Clustering of self-propelled particles

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Many experimental realizations of self-propelled particles exhibit a strong tendency to aggregate and form clusters,[1][2][3][4][5] whose dynamics are much richer than those of passive colloids. These aggregates of particles form for a variety of reasons, from chemical gradients to magnetic and ultrasonic fields.[6] Self-propelled enzyme motors synthetic nanomotors also exhibit clustering effects in the form of chemotaxis. Chemotaxis is a form of collective motion of biological or non-biological particles toward a fuel source or away from a threat, as observed experimentally in enzyme diffusion[7][8] and also synthetic chemotaxis[9][10][11] or phototaxis.[11] In addition to irreversible schooling, self-propelled particles also display reversible collective motion, such as predator-prey behavior and oscillatory clustering and dispersion.[12][13][14]

Phenomenology

This clustering behaviour has been observed for self-propelled Janus particles, either platinum-coated gold particles[1] or carbon-coated sillica beads,[2] and magnetically or ultrasonically powered particles,[5][6] as well as for colloidal particles with an embedded hematite cube[3] and composed of slowly-diffusing metal ions,[4][12][13][14] and for enzyme molecule diffusion.[7][8] In all these experiments, the motion of particles takes place on a two-dimensional surface and clustering is seen for area fraction as low as 10%. For such low area fractions, the clusters have a finite mean size[1] while at larger area fractions, larger than 30%, a complete phase separation has been reported.[2] The dynamics of the finite-size clusters are very rich, exhibiting either crystalline order or amorphous packing. The finite size of the clusters comes from a balance between attachment of new particles to pre-existing clusters and breakdown of large clusters into smaller ones, which has led to the term of "living clusters".[3][4][12][13][14]

Mechanism for synthetic systems

The precise mechanism leading to the appearance of clusters is not completely elucidated and is a current field of research.[15] Three different mechanisms have been proposed, which could be at play in different experimental setups.

First, self-propelled particles have a tendency to accumulate in region of space where they go slower;[16] then, self-propelled particles tend to go slower where they are denser, because of steric hindrance. A feedback between these two mechanisms can lead to the so-called motility induced phase separation.[17] This phase separation can however be arrested by chemically-mediated inter-particle torques[18] or hydrodynamic interactions,[19][20] which could explain the formation of finite-size clusters.

Alternatively, clustering and phase-separation could be due to the presence of inter-particle attractive forces, much as in equilibrium suspensions. Active forces would then oppose this phase separation by pulling apart the particles in the cluster,[21][22] following two main processes. First, single particles can evaporate if their propulsion forces are sufficient to escape from the cluster. Then, a large cluster can break into smaller ones due to the build-up of its internal stress: as more and more particle enter the cluster, their propulsive forces add up until they break down its cohesion. Diffusiophoresis is also a commonly cited mechanism for clustering and collective behavior, involving the attraction of particles to each other and in response to ion gradients.[4][12][13][14] Diffusiophoresis is a process involving the gradients of electrolyte or non-electrolyte concentrations interacting with charged or neutral particles in solution and with the double layer of any walls or surfaces.[14]

In experiments, arguments have been put forward in favour of both mechanisms. For carbon-coated sillica beads, attractive interactions are supposed to be negligible and phase-separation is indeed seen at large densities.[2] For other experimental systems, attractive forces could however play a larger role.[1][3][4][12][13][14]

Reviews

Clustering behavior in self-propelled particles and enzyme motors is discussed in great detail in sections on Collective Behavior, Chemotaxis, and/or Diffusiophoresis within several reviews by leading researchers in the self-propelled particles and nanomotors fields.[23][24][25][26][27]

References

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